by treating separately the elastic and the surface energy. For the latter we employ a blow-up method differently performed for each portion of the \(\partial A\)  where \(\widetilde{\psi }\)  is supported. In particular extra care is needed for the jump set \(J_u\)  and jump set along cracks \(S_u^A\)  (since there is no bound on the number of connected components), where we need to extend some ideas from [1]}.
